Lecture 14 Magnetic Circuits An electromagnetic-mechanical system is formed with the following blocks. We know that the integral form of Ampere’s Law is CSH dlJ dS=∫∫iiL. Considering the next figure, an iron core with cross-sectional area A and with mean length of perimeter l, several assumptions were made: Ampere’s Law Material properties Faraday’s Law Ohm’s Law, KCL, and KVL Lorenz’s Law and energy conservationNewton’s and Lagrange’s Laws Speed, displacement e B, ΦH i
has intentionally blurred sections.
Sign up to view the full version.